Ioniser for use in a cycloidal mass spectrometer

Abstract: A Cycloidal mass Spectrometer having a housing (2) which defines an ion trajectory volume (4), an electric field generator for establishing an electric field within the ion trajectory volume (4) and an ioniser (8) for receiving gaseous specimens to be analysed and converting the same into ions which travel through magnetic fields and impinge upon a collector (12). The ioniser comprises an ion volume having a gas inlet opening for introducing a gaseous specimen into the ion volume and filament means. The ion volume has an ioniser volume block composed of ceramic material. The cycloidal mass spectrometer and the ioniser may be miniaturised.

Description: The present invention relates to an improved ioniser which may be used in a cycloidal mass spectrometer and, more specifically, it relates to such apparatus which readily may be miniaturized. The use of mass spectrometers in determining the identity and quantity of constituent materials in a gaseous, liquid or solid specimen has long been known. It has been known, in connection with such systems, to analyze the specimen under vacuum through conversion of the molecules into an ionic form, separating the ions by their mass to charge ratio, and permitting the ions to bombard a detector. See, generally, U.S. Patent Nos. 2,882,410; 3,070,951; 3,590,243; 4,298,795. See, also U.S. Patent Nos. 4,882,485 and 4,952,802. In general, ionisers contain an ioniser inlet assembly wherein the specimen to be analyzed is received, a high vacuum chamber which cooperates with the ioniser inlet assembly, an analyzer assembly which is disposed within the high vacuum chamber and is adapted to receive ions from the ioniser. Detector means are employed in making a determination as to the constituent components of the specimen employing mass to charge ratio as a distinguishing characteristic. By one of many known means, the molecules of the gaseous specimen contained in the ioniser are converted into ions which are analyzed by such equipment. It has been known with prior art cycloidal mass spectrometers to use a single fixed collector and ramped electric field in looking at only one mass to charge ratio at a time. In known mass spectrometer systems, whether of the cycloidal variety type or not, the ionisers are quite large and, as a result, dominate the design and specifications of the systems to be employed therewith. In spite of the foregoing system, there remains a very real and substantial need for an improved cycloidal mass spectrometer and for ionisers used therewith and with other types of mass spectrometers. US-A-4206383 discloses a miniature ion source device particularly for use in an ion cyclotron resonance mass spectrometer. The ion source device comprises an ioniser chamber partly defined by a pair of spaced apart side walls, each having an aperture therethrough. Electrons pass in a beam through the apertures from a wire filament located outside the ioniser chamber, to a collector also located outside the chamber. EP-A-0346271 discloses a miniature field ioniser which is generally planar in configuration, comprising an array of small diameter gas outlets in the form of microvolcanos. Each gas outlet, or more particularly the rim thereof, is defined by a layer of an electrically conductive material capable of maintaining an electrical potential. It is an object of the present invention to provide a miniaturised ioniser which is usable within a cycloidal mass spectrometer and in other systems wherein ion generation is needed. It is another object of the present invention to provide a miniaturised ioniser which can operate at pressures higher than normally considered ideal while making ionization more efficient. According to the present invention, there is provided ioniser means for a mass spectrometer; the ioniser means comprising an elongate ioniser volume block of a ceramic material defining a recess, the block cooperating with a plate to define an ioniser chamber, the plate having an exit slot therein; and filament means within said ioniser chamber adapted to be supplied with electricity, wherein the ioniser means has an exterior length of less than 12,7 mm (½ inch). Preferably, the filament means comprises a wire filament within said ioniser chamber, whereby the filament may be heated to incandescence by electrical resistance heating. Advantageously, the filament means comprises an electrically conductive coating on the interior surface of the ioniser volume block, and there being provided means to apply voltages to said coating to produce electric fields. Conveniently, the ioniser means further comprises a gas inlet opening for introducing gaseous specimens into the ioniser chamber. Preferably, the gas inlet opening is disposed at one end of the ioniser volume block and the wire filament is disposed at the other end of the ioniser volume block. Advantageously, the exit slot is disposed at a position along the length of the ioniser volume block between the gas inlet opening and the wire filament. Conveniently, the recess is defined by a channel formed in the ioniser volume block, the ioniser volume block being provided with two end walls. Preferably, the ioniser means has an exterior width of about 1.6 mm to 4.8 mm (1/16 to 3/16 inch) and an exterior height of about 4.8 mm to 7.9 mm (3/16 to 5/16 inch) each. Advantageously, the ioniser means has an exterior length of about 4.8 mm to 12,7 mm, (3/16 to 1/2 inch). These and other objects of the invention will be more fully understood from the following detailed description of the invention on reference to the illustrations appended hereto. Figure 1 is a schematic cross-sectional illustration of the ion trajectory volume of a cycloidal mass spectrometer in which the ioniser means of the present invention can be used, Figure 2 is a perspective view of the exterior of the cycloidal mass spectrometer, Figure 3 is a vertical cross-sectional illustration of the cycloidal mass spectrometer of Figure 2 taken through 3-3, Figure 4 shows a form of the cycloidal mass spectrometer of Figure 2 positioned between the two poles of magnetic field generating means, Figure 5 is an exploded view of a form of collection means of the mass spectrometer, Figure 6 is a schematic illustration of one possible arrangement of collection means, Figure 7 is an exploded view of a second possible arrangement of collection means, Figure 8 is a schematic illustration of a third possible arrangement of the collection means, Figure 9 is an exploded view of the miniaturized ioniser of the present invention, Figure 10 is a top plan view of the miniature ioniser of Figure 8 without the injector plate in place, Figure 11 is a schematic illustration of a modified form of cycloidal mass spectrometer, Figure 12 is a schematic illustration of the mass spectrometer of Figure 11 and its associated enclosure, and Figure 13 is a top plan view of the spectrometer of Figure 11. While the actual path of movement of the ions in the mass spectrometer disclosed herein might best be described as a "trochoid", it has been accepted in the art to refer to such a mass spectrometer as a "cycloidal mass spectrometer" and this latter term is being employed herein. Referring once again to Figure 1, there is shown a cycloidal mass spectrometer which has a housing 2 defining an ion trajectory volume 4 in which is a magnetic field having its B field going into the drawing and the plate produced E field going perpendicular to the B field and toward the top of the page. The magnetic field establishes flow of the ion beam 6 which emerges from the ioniser means 8. The ion beam 6 splits according to ion mass to charge ratio and impinges upon different portions of the collection means 12 with the ions of lesser mass impinging upon the collection means 12 at a distance closer to the ioniser 8 than those ions of greater mass. It will be noted that the collection means 12 receives a plurality of ions having different mass to charge ratios simultaneously. Impingement of the ions on the collection means 12 causes a responsive current to flow through leads 14 to processing means 16 wherein determinations are made as to the mass distribution of the ions in ion stream 6. This permits a quantitative and qualitative determination of the materials present in the gaseous sample which was introduced into the ioniser means 8. Referring still to Figure 1, there is shown a plurality of circumferential electrically conductive metal electric field plates 20, 22, 24, 26 which are electrically separated from each other by electrically insulating material 28, 30, 32 which may be ceramic, glass, a low vapor pressure polymer, or combinations thereof. Where the plates 20, 22, 24, 26 (apart from the electrically conductive coatings applied thereto) are made of electrically insulative materials, the materials per se may function as the insulating material without using a separate material. In the arrangement where the plates 20, 22, 24, 26 are composed of an electrically insulative material such as alumina, for example, the lower surface and a circumferentially continuous lower portion of the inner surface of a plate will be coated with an electrically conductive material. The upper surface of the plate and a circumferentially continuous upper portion of the inner surface of the plate will be coated with an electrically conductive material. A gap will be left between the upper and lower inner coated portions. The upper surface of one plate may be joined to the lower surface of an overlying plate by suitable means, such as brazing, for example, to provide a sealed joint therebetween. In this manner, the electrical field plates 20, 22, 24, 26 cooperate to define the ion trajectory volume 4 which is under vacuum. The "ion trajectory volume" is a space within the field plates in which the analyzed ions travel from the ion source exit slit to the focal plane. Any desired number of such plates may be employed in defining the electric field forming section of the cycloidal mass spectrometer housing. As the electric field plates are sealed, there is no need to employ a separate vacuum chamber. As shown, with reference to Figures 1 through 3, the plate defined, ion trajectory volume 4, is in the lower portion of the housing 2 of the cycloidal mass spectrometer. Housing 2 tapers generally upwardly and communicates with opening 42 of the flanged upper portion 44 so as to permit connection to a suitable vacuum pump (not shown). As shown in Figure 2, the collector plates indicated generally as 46, 48, 50, 52, 54, 56 may be provided in any desired number depending on the ultimate resolution desired. In Figure 3, the array of vertical stacked plates 58a through 58p are, in the form shown, generally rectangular in external peripheral configuration and have a generally rectangular opening therein. The upper plates 58a through 58k are generally of the gaseous the same size and shape and have aligned openings of the same size. The lower plates 581 through 58p are each of generally the same size and shape and have aligned openings of the same size. Each plate 58a-58p has its own electrical supply wire 60a through 60p to supply electricity thereto. A gas inlet 62 supplies the gaseous sample to be analyzed to ioniser 8 (Fig. 1). The processing means 16 receive electrical signals from the collection means 12 (Fig. 2) by electrical leads 14. As shown in Figures 2 through 4, the generally flat parallel opposed surfaces 61, 63 of the housing 2 are positioned between the poles 62, 64 of permanent magnet 66 or an electromagnetic so as to place the electric field plates within the magnetic field generated between poles 62, 64. As shown in Figure 1, the ions emerging from ioniser means 8 travel to the collection means 12 under the influence of this magnetic field. Referring to Figure 5, there is shown an exploded view of a form of electric field plate arrangement. These plates in the preferred arrangement are composed of an electrically nonconductive, nonporous ceramic material such as high density alumina, which may be coated on the upper and lower surfaces and interior surface, (with gaps as described hereinbefore) which is exposed to the ion trajectory volume 4, with a suitably electrically conductive material such as molybdenum, molybdenum-manganese, nickel and copper, for example. Adjacent electrically conductive coatings will be electrically insulated from the adjacent electrically conductive coatings on the plates. The filament plate 68 is the uppermost plate and in the form shown is generally rectangular in shape and defines a rectangular opening 69. Underlying filament plate 68 and adapted to be separated therefrom by electrically insulative material is ioniser plate 70 within which ioniser 8 is positioned with its injector plate 74 having an elongated slit 76 secured to the undersurface thereof. The gaseous specimen enters ioniser 8 through gas inlet 62 which extends through a metallized passageway 72 in plate 70. The gas inlet tube 62 preferably serves to not only introduce the gaseous specimen into the ioniser, but also serves to place voltage on the repeller. The electrically energized filament 65 is secured to filament plate 68 and is received within recess 67. It will be appreciated that in this manner ions generated in the ioniser means 8 from the gaseous specimen introduced thereinto, by means to be described hereinafter, will be discharged in a generally downward direction within the short leg 80 (See Figs. 1 and 2) of the ion trajectory volume 4. It will be appreciated that the ioniser means 8 is disposed within opening 82 defined by plate 70 and is in spaced relationship with respect to interior end 84 of the opening 82. The collection means includes collection plate 88 and associated overlying apertured plate 90. Collection plate 88 is generally rectangular in shape and is preferably of essentially the identical shape and size as plates 68, 70. The opening 92 defined within collection plate 88 has a plurality of detectors 94, 95, 96, 97, 98, 99, 100 which underlie and are operatively associated with generally parallel slits 104, 106, 108, 110, 112, 114, 116, in apertured plate 90 which is disposed in the focal plane. Slit 118 is aligned with slit 76 of injector plate 74 and serves as ion entrance slit to the cycloidal system. Referring to Figures 1 and 5, it will be appreciated that ions traveling in beam 6 will impinge upon various portions of apertured plate 90 but will pass through only those portions of the apertured plate 90 wherein the generally parallel slits 104, 106, 108, 110, 112, 114, 116 are present. The ions passing through these slits will impinge upon the underlying detectors 94, 95, 96, 97, 98, 99, 100 and produce a plurality of responsive currents which will be received by processing means 16 through electrical leads 14 (Fig. 1) and be processed in such a manner to provide the desired information as to the quantitative and qualitative content of the major ingredients of the gaseous specimen. This information might be stored in a computer, visually displayed on an oscilloscope, provided in hard copy, or handled in any other desired manner. Figure 6 shows a detailed illustration of one arrangement of the portion of the collection means shown in Figure 5. The apertured plate 90 has its slits 104, 106, 108, 110, 112, 114, 116 each overlying one of the detectors 94, 95, 96, 97, 98, 99, 100. In a preferred arrangement the collectors 94, 95, 96, 97, 98, 99, 100 are Faraday plate ion collectors. Each collector's current may be read in the processing means 16 by a separate amplifier (not shown) in a manner well known to those skilled in the art or, in the alternative, a single amplifier and a multiplexing system may be employed. In this arrangement the apertured plate 90 may be made of stainless steel having a thickness of about 0.05mm (0.002 inch). It is also preferred that the orientation of the slits 104-118 (even numbers only) be not only parallel to each other, but also parallel to the slit 76 in the ioniser means injector plate 74 (Fig.5). The slits preferably have a width of about 0.076 mm (0.003 inch). As will be apparent, the positioning of the slits will be determined by what specific ion masses that are to be observed. It will be appreciated that this system permits detection of a plurality of ions of different mass to charge ratios simultaneously and thereby provides a highly efficient means of analysing a gaseous specimen. In this arrangement as well as the other arrangements of collection means 12, it is preferred that the entrance to the apertured plate 90 be preferably positioned generally in the focal plane of the apparatus. Considering Figure 7, a second arrangement of the collection means will be considered. An array of collectors of a charged coupled device is employed. In this embodiment, the ion current activates the charged coupled device 119 due to direct or induced ion current coupling to the array of the charge collectors. The entire mass spectrum may be employed or, in the alternative, only isolated desired parts of the mass spectrum may be employed. Also, if desired, resolutions higher than those that may be obtained in the static mode may be achieved by dithering the electric field and monitoring the signals to the collectors as a differential in time. The charge coupled device 119 may have the charge coupled array directly established on the ceramic material of plate 88' or may be created as a separate entity and secured to the plate 88'. The second arrangement of collection means, as shown in Figure 7, eliminates the apertured plate and ion charges are collected directly or induce a charge directly on the array. As prior art systems employ photons which are capable of traveling through nonconductive materials, these systems are not desirable for direct ion detection. Referring to Figure 8, a further arrangement of the collection means will be considered. In this arrangement, underlying the apertured plate 90 is a channel plate 130 under which a plurality of detectors 132-138 are provided in aligned position with respect to slits 104-116 (even numbers only). The channel plate 130, which may be a leaded glass channel plate, is preferably positioned just below the focal plane of the cycloidal mass spectrometer. As the focal plane is at ground potential and the front of the channel plane must be at a high negative potential, the focal plane is occupied by a plate 90 which in this arrangement is a grounded metal screen provided with the slits 104-118 (even numbers only). Due to the high magnetic field involved, channel diameters of less than 10 microns are preferably used. In this channel plate arrangement, an ion hits on the leaded glass channels and cause a number of secondary electrons, each of which are accelerated down the channel to produce more electrons, this cascading process produces the amplification. The current going to the detectors 132-138 will be an electron current and will have a magnitude about four orders of magnitude higher than the ion current. The processing means 16 will then process the electrical signals. Referring now to Figures 9 and 10 an ionizing means 8 of the present invention will be considered in greater detail. It will be appreciated that while the miniaturized ioniser means of the present invention are adapted to be used in the portable cycloidal mass spectrometer described above, it may be used in other installations where it is desired to convert a gaseous specimen to ions. The ion volume block 150 is preferably composed of an electrically insulative, substantially rigid material which will be inert to the gaseous specimens to be reintroduced therein. Among the suitable materials for such use are high density alumina, preferably of about 94 to 96 percent purity. The ion volume block 150 is elongated and has a pair of upstanding, generally parallel sidewalls 152, 154, a base 169 and a pair of endwalls 158, 160. These cooperate to define upwardly open recess 164. Formed within the endwall 158 is a gaseous specimen introducing opening which cooperates with gas inlet tube 180. The portion of the sidewalls 152, 154 adjacent to endwall 160 have shoulders 170, 172. In this portion of the base 156, which serves as the filament plate, is a filament 177 which may be a wire filament which may be made of tungsten, thoria coated indium or thoriated tungsten, for example. It is supported by posts 178, 179. The filament 177 is preferably electrically energized by a suitable wire, (not shown) to effect resistive heating to incandescence by currents on the order of a few amps. The filament 177 may be a ribbon about 0.025mm (0.001 inch) thick, about 0.13mm (0.005inch) wide and about 2.5mm (0.1 inch) long. The generally channel shaped body portion or block 150 cooperates with endwalls 158, 160 and the injector plate 76 to define the ioniser chamber. In lien of using filament 177, the ioniser volume block 150 may have its interior surface coated with a suitable electrically conductive metal which is electrically energized. The electric fields are produced by applying voltages to the metal coated ceramic high density alumina walls. The metal coating on the ceramic produces equal potential surfaces and conductive traces which allow the surface potentials to be applied from outside the device. Inlet tube 180 which receives specimen gases from inlet tube 62 by means of the connecting passageway (not shown) for introduction of the gas specimen is in communication with recess 164. Inlet tube 180 is disposed at the opposite end of recess 164 from filament 177 and exit slot 76 is disposed between such ends. Suitable means for introducing a gaseous specimen into the inlet, tube 62 is disclosed in co-pending United States Application Serial No. 071911,469, filed on July 10, 1992 in the names of Kurzweg and Duryea and entitled "Inlet Valve Apparatus for Vacuum Systems". The ioniser means 8 also has injector plate 74 positioned with its slot 76 generally parallel to the longitudinal extent of the ion volume block 150. In the preferred embodiment of the invention the ioniser means will have an exterior length of about 4.8 to 12,7mm (3/16 to 1/2inch), an exterior width of about 1.6 to 4.8mm (1/16 to 3/16 inch) and an exterior height of about 4.8 to 7.9mm (3/16 to 5/16 inch). The ioniser means has an interior passageway having a length of less than about 5mm (1/5 inch). The mean free paths between electron-molecule collisions at about 10 microns of pressure are about this length. As a result, these devices will function efficiently at these pressures. It will be appreciated that in this manner this compact ioniser may be employed in a very small space within a mass spectrometer and thereby contribute to reduction in size, and provide portability and enhanced efficiency. The cycloidal mass spectrometer useful with the ioniser mean of the present invention preferably has an interior which has a height of about 25 to 76mm (1 to 3 inches), a width of about 9,5 to 16mm (3/8 to 5/8 inch)and a depth of about 51 to 102mm (2 to 4 inches). The ion trajectory volume preferably has an interior length of about 38 to 51mm (1.5 to 2.0 inch), an interior width of about 7.6 to 17,8mm (0.30 to 0.70 inch) and an interior height in the region of the collector means of about 15 to 38mm (0.6 to 1.5 inch). It will be appreciated that electrons emerging from the filament 177 are accelerated within the ion volume by a potential difference between the filament 177 and the ion volume potential. These potentials are applied by voltage sources disposed outside of the analyzer assembly and are directed to the applied location by means of the metallic coating traces on the ceramic plates. These electrons are entrained to move within the ion volume by a magnetic field which may be on the order of about 4000 Gauss. It will be appreciated that the specimen gas to be evaluated is introduced directly into the ion volume and is provided with no major exit path other than the aperture 76 in the injector plate 74. Ions are extracted from the ioniser by the combined potentials of the injector and the ion volume potential. It will be appreciated while the injector plate 74 is shown with elongated linear slit 76 in some uses slits having a different shape may be desired and employed. It will be appreciated that by employing ioniser means 8 of such small size the ioniser may be placed within or in close proximity to the analysing magnets that establish the magnetic field. The analysing magnet as a result, produces a field which also serves as the electron beam confining field. The magnetic field is placed parallel to the electron beam direction. Any component of electron velocity away from a magnetic field line will cause the electron to circle the field line. As a result, the magnetic field confines and directs the electron beam. If no magnetic field already exists, an ioniser magnet positioned so that its field lines are in the direction of the electron beam can be employed to improve performance. The apparatus described above is double focusing in that ions of one mass to charge ratio focus at one place on the collection means regardless of the initial ion energy spread or a spread in the ion injection angle. It will be appreciated that the apparatus facilitates the use of miniaturized portable equipment which will operate with a high degree of efficiency and permit simultaneous impingement of the plurality of ions on the collection means 12 thereby facilitating measurement of ions of different mass to charge ratios simultaneously. It will further be appreciated that all of this is accomplished using a unique ioniser means which is suitable for use in the apparatus disclosed herein as well as other apparatus wherein conversion of gaseous specimen to ions is desired. Another advantage to the construction described above is that it allows the vacuum system/ion trajectory volume to be more narrow than other cycloidal mass spectrometers. The system also operates with a magnetic field gap which is about one-half the width that would normally be required if separate field plates and vacuum walls were employed. The apparatus employs a very uniform magnetic field the magnet gap width of which will generally be rather small such as of the order of about 9,5 to 16mm (3/8 to 5/8 inch), thereby facilitating the use of magnets which are much smaller. Numerous end uses of the cycloidal mass spectrometer, and the ioniser means of the present invention, will be apparent to those skilled in the art. Among such uses will be efforts to determine purity of air in order to comply with legislation establishing requirements therefor, auto exhaust gas analysis, uses in analytical chemistry such as in gas chromatography mass spectrometry and uses in the medical fields, such as in an anaesthetic gas monitor. It will be appreciated that the apparatus measures the mass to charge ratio of a plurality of ions impinging on collection means simultaneously. Also, unique electric field plates serve to define the ion trajectory volume. In addition, unique ioniser means, which may be of very small size, are provided. While a preferred feature of the mass spectrometer provides a plurality of field plates, each coated on the interior with electrically conductive traces, it will be appreciated that, if desired, the ion volume may be defined by a unitary molded structure made from a low vapor pressure elastomer such as a suitable rubber or plastic. A suitable material is that sold under the trade designation "Kalrez" by E.I. DuPont de Nemours. The unitary construction may be made of the same size and configuration as the assembled array of plates and have the electrically conductive tracings applied thereto. Referring to Figures 11 and 12, an additional arrangement will be considered. Whereas, in the prior arrangement emphasis has been placed upon the use of ceramic or other electrically non-conductive material having coated thereon electrically conductive traces and having such construction sealed to define the ion volume, the present arrangement takes a different approach. More specifically, it contemplates the use of a plurality of electrically conductive plates which are electrically insulated from each other and the use of a separate vacuum enclosure to receive the assembly of plates. The plates may generally be of the same configuration and dimensions as those discussed hereinbefore. The array of negative plates 200-218 (even numbers only) are disposed in relative spaced relationship to each other. A series of positive plates 226, 228, 230, 232 are disposed in relative spaced relationship to each other. The positive plates have threaded rods 240 and 242 passing through openings therein with a plurality of electrically insulative washers 250-270 (even numbers only) , have rod 240 pass therethrough, and serve as spacers between the respective plates 200-218 (even numbers only). As shown in Figure 13 and described in greater detail hereinafter, rods 400, 402 which are similar to rods 240, 242 and disposed, respectively, in spaced relationship to rods 240,242. The washers may conveniently be made of alumina and be about 0.6mm (0.024 inch) thick. The washers 250-270 (even numbers) preferably extend about 0.38mm (0.015 inch) beyond the stack and serve to insulate the plates from the metal surfaces of the vacuum envelope which will be described hereinafter. Nuts 274, 280 serve to secure mounting brackets 276, 282 and secure the assembly of plates 200-218 (even numbers only) . Similarly, threaded rod 242 passes through a plurality of washers 290-310 (even numbers only) to provide spacing and insulation between the respective plates 200-218 (even numbers only). Also, washers 320-328 (even numbers only) have rod 242 passing therethrough and separate positive plates 226-232 (even numbers only). Nuts 332, 334 are threadedly secured to rod 242 and establish the assembly. The ioniser 340 and filament assembly 342 are interposed between the negative plates 200-218 and positive plates 226-232. The individual potentials of plates 200-218 and 226-232 are distributed by means of a plurality of vacuum compatible resistors 350-376 (even numbers only) which are used as a voltage dividing resistor chain. The resistors are preferably spot-welded to the plates 200-218 and 226-232 and form an integral part of the flange mounted assembly. In this arrangement, the electric field plates 200-218 and 226-232 are made of stainless steel and preferably annealed 304 stainless steel, having a thickness of about 1.8mm (0.072 inch). The rods 240, 242 are preferably 56 304 stainless steel threaded rods insulated with exteriorly disposed alumina tubing. As this arrangement does not have the sealed plates as described in the ceramic arrangement hereinbefore described, this arrangement employs a separate vacuum enclosure 360 (Figure 12) within which the assembly of steel plates is received. The vacuum enclosure 360 is preferably formed of 304 stainless steel tubing which may be shaped by a mandrel and have vacuum flanges 362, 364 welded to opposed ends. The flange 362 may be secured to front plate 366 by a plurality of Allen Head Machine Screws (not shown) which secure flange 362 to front plate 366 in order to establish a vacuum seal therebetween. The flange 364 may be secured in a vacuum tight seal to the ion pump 368 by a plurality of machine screws. The vacuum seal is created by crushing a metal 0-ring made of silver-tin, copper or aluminum, for example, between flange 362 and front plate 366 with tightening being effected by the screws. The front plate 366 may be secured to the mounting brackets by screws such as 396, 398 in Figure 13 or spot welding, for example. It will be appreciated that in this manner, in this arrangement, the vacuum chamber is defined by the vacuum enclosure 360, rather than being formed integrally with the plates defining the same. This arrangement otherwise functions in the same manner as the prior arrangement. The ion source within the ioniser 340 may either be made as previously described herein, or may be made of stainless steel, such as 304 stainless steel and coated with a low vapor pressure insulating polymer on its inside surface. A suitable polymer for this purpose is varian "Torr Seal." The vacuum feedthrough allows for the passage of positive plate potential, negative plate potential, filament current end filament potentials, repeller potential, and gas from atmospheric pressure to high vacuum. These electronic currents and potentials may originate in the electronics unit (not shown) and pass into a high vacuum. When the plate assembly, secured to the front plate 366, is placed within the vacuum enclosure 360, the vacuum enclosure is compression sealed by use of metal gaskets which are disposed between the flanges which are secured by Allen Head Screws. As is shown in Figures 11 and 12, the plates 202-218 and 226-232 have a generally rectangular central opening as represented on each plate by a pair of spaced vertically oriented parallel dotted lines. The top plate 200, in the form shown, does not have such an opening. As shown in Figure 13, the mounting bracket 276 is secured to plate 366 by screws 396, 398. Bracket 282 may be secured to plate 316 in the same manner. Rods 240, 400 pass through mounting bracket 276 and the underlying plates 200-218 and are secured at their upper ends by nuts 274, 404 respectively, and other nuts (not shown) at the lower ends of rods 240, 400. Similarly, rods 242, 402 pass through plates 200-228 and 226-232 and are secured at their upper ends by nuts 242, 402 respectively, and other nuts (not shown) at the lower ends of rods 242, 402. In order to resist undesired electrical contact between the plates 200-218, 226-232, and the interior of vacuum enclosure 360, electrically insulative washers 252-270 and 322-328, such as 252 and 292 shown in Figure 13 are preferably continuous and rectangular and have their ends projecting beyond plate sides 410, 412. The washers preferably have a thickness of about 0.76 to 0.51mm (0.030 to 0.020 inch),a length of about 12,45 to 12,7mm (0.490 to 0.500 inch) and a width of about 4.6 to 5.6mm (0.18 to 0.22 inch). Whereas particular embodiments of the invention have been described herein for purposes of illustration it will be evident to those skilled in the art that numerous variations of the details may be made without departing from the invention as set forth in the appended claims.

Claims: Ioniser means for a mass spectrometer, the ioniser means comprising an elongate ioniser volume block (150) of a ceramic material defining a recess (164), the block cooperating with an injector plate (74) to define an ioniser chamber, the injector plate (74) having an exit slot (76) therein, filament means within said ioniser chamber adapted to be supplied with electricity, the ioniser means having an exterior length of less than 12,7 mm. Ioniser means according to claim 2, wherein the filament means comprises a wire filament (177) within said ioniser chamber, whereby the filament (177) may be heated to incandescence by electrical resistance heating. Ioniser means according to claim 1, wherein the filament means comprises an electrically conductive coating on the interior surface of the ioniser volume block (150), and there being provided means to apply voltages to said coating to produce electric fields. Ioniser means according to any preceding claim, further comprising a gas inlet opening (180) for introducing gaseous specimens into the ioniser chamber. Ioniser means according to claim 4 as dependent upon claim 2, wherein the gas inlet opening (180) is disposed at one end of the ioniser volume block (150) and the wire filament (177) is disposed at the other end of the ioniser volume block (150). Ioniser means according to claim 5, wherein the exit slot (76) is disposed at a position along the length of the ioniser volume block (150) between the gas inlet opening (150) and the wire filament (177). Ioniser means according to any preceding claim, wherein the recess (164) is defined by a channel formed in the ioniser volume block (150), the ioniser volume block (150) being provided with two endwalls (158,160). Ioniser means according to any preceding claim having an exterior width of about 1.6mm to 4.8mm and an exterior height of about 4.8mm to 7.9mm. Ioniser means according to any preceding claim having an exterior length of about 4.8mm to 12,7mm.

Inventors: KURZWEG LUTZ, KURZWEG, LUTZ
Applicants: MONITOR INSTR CO LLC, MONITOR INSTRUMENTS CO, LLC
Application year: 1994
Main classification: H01J49
IPC codes: H01J49